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Numerical modelling of a dual-rotor marine current turbine in a rectilinear tidal flow

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In this paper, numerical simulation is used to investigate a counter-rotating dual-rotor marine current turbine (MCT) that is aligned for a rectilinear tidal current, and results of power and thrust coefficients and the mean axial velocity in the wake are compared with that of the blade element momentum (BEM) method coupled with the Park wake model.
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This article is published in Ocean Engineering.The article was published on 2020-03-15 and is currently open access. It has received 6 citations till now. The article focuses on the topics: Rotor (electric) & Turbulence kinetic energy.

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Citations
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Velocity interference in the rear rotor of a counter-rotating wind turbine

TL;DR: In this article, a counter-rotating wind turbine with two rotors rotating in opposite directions on the same axis is proposed to improve the aerodynamic performance of a wind turbine.
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Optimization of the hydrodynamic performance of a vertical Axis tidal (VAT) turbine using CFD-Taguchi approach

TL;DR: In this article, a number of CFD simulations have been carried out using the mixed-level modified Taguchi technique to determine the optimal hydrodynamic performance of a VAT turbine, and the influence of four parameters: twist angle, camber position, maximum camber, and chord/radius ratio has been studied.
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Study on two-rotor interaction of counter-rotating horizontal axis tidal turbine

- 01 Feb 2022 - 
TL;DR: In this paper , a numerical model based on large eddy simulation (LES) is established to study the hydrodynamic performance of a two-rotor turbine, and it is validated by a flume experiment.
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Coaxial horizontal axis hydrokinetic turbine system: Numerical modeling and performance optimization

TL;DR: In this paper, the authors derived the optimum design criteria for a coaxial horizontal axis hydrokinetic turbine system utilizing both numerical and experimental approaches, and then extended the numerical modeling to analyze the performance of the coaxial multi-turbine system.
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Numerical Study of A Generic Tidal Turbine Using BEM Optimization Methods

TL;DR: In this paper, three blade geometry optimization models derived along with assumptions from the blade element momentum (BEM) approach are studied by using a steady BEM code to improve a small horizontal-axis rotor of three blades.
References
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A note on wind generator interaction

TL;DR: In this article, a simple wake model for the wake behind a wind generator is given, and the model is compared to some full scale experimental results, where the production from a circular cluster of 10 wind generators is calculated.
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A Model-Free Approach to Wind Farm Control Using Game Theoretic Methods

TL;DR: It is demonstrated that this learning rule can provably maximize energy production in wind farms without explicitly modeling the aerodynamic interaction amongst the turbines.
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Experimental study of the turbulence intensity effects on marine current turbines behaviour. Part I: One single turbine

TL;DR: In this paper, the authors show that while the wake of the turbine is deeply influenced by the ambient turbulence conditions, its mean performances turn out to be slightly modified, which is crucial in the view of implanting second generation turbines arrays.
Journal ArticleDOI

Wind turbine wake models developed at the technical university of Denmark: A review

TL;DR: In this article, six widely used approaches of wake modelling (Jensen, Larsen, Dynamic Wake Meandering, Fuga and, Ellipsys3D LES and RANS together with their interpretations) are described and the model subcomponents are analyzed.
Journal ArticleDOI

Experimental study of the turbulence intensity effects on marine current turbines behaviour. Part II: Two interacting turbines

TL;DR: In this paper, the authors focus on the interactions between two horizontal axis marine current turbines, axially aligned with the upstream flow, and characterise the wake of each turbine so as to explain their behaviour.
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Frequently Asked Questions (17)
Q1. What are the contributions in "Numerical modelling of a dual-rotor marine current turbine in a rectilinear tidal flow" ?

In this study, numerical simulation is used to investigate a counter-rotating dual-rotor marine current turbine ( MCT ) that is aligned for a rectilinear tidal current. 

For a single-rotor tip-pitched at θT = −2◦, a high turbulence intensity region (such as TI > 0.28) extends to 5D downstream after the rotor and 0.6D in radial direction, while the high turbulence intensity region is mainly340 constrained near the hub for a single-rotor tip-pitched at θT = 2 ◦. 

The unsteady RANS simulation can also be used to improve the prediction of performance and load on rear rotor which operates in turbulent windmill state and experiences370 larger fluctuations during one periodic cycle. 

At low305 TSRU (2.91, 3.75), there are large flow separation from the rear surface of the blade, while no flow separation is observed at high TSRU , such as TSRU = 6. 

The LSB is near the inner board of blade and thickens the boundary layer, thus contributes to the295 decrease of profile hydrodynamic efficiency, CL/CD. 

Due to higher waterproof standard, the electrical pitch system for tidal turbine is more expensive and vulnerable than that of a wind turbine which normally operates in a dry environment [2]. 

The power coefficient of the E387 rear rotor was found to be highly negative, less than - 0.5 for TSR = 4 when using RANS or BEM, hence justifying again the use of the symmetric profile NACA0012 for180 the dual rotor configuration. 

The vortex size is about 0.5D for a single-rotor tip-pitched at θT = 2◦, while a much larger size of vortex (6D) is observed for a single-rotor tip-pitched at θT = −2◦. 

Based on the CT of front rotor and area-averaged axial mean velocity from RANS results, the calibrated value of k is 0.017( TI=15%) using the least square fitting [36]. 

the optimum TSR of the NACA0012 rotor (θT = 2◦) is about 4.75, which is higher than that of the E387 turbine (TSR=4.25) [29]. 

The vortical wake shedded by the front rotor is seen to reduce the wake behind the rear rotor compared to the single-rotor wake and thus has the potential actually to mildly increase the rear315 rotor hydrodynamic efficiency, explaining the high CP seen in Fig. 9 (b). 

The power coefficients of front and rear rotor of a dual-rotor turbine are190 denoted as Cfrontp,dual and C rear p,dual, respectively. 

For a single-rotor tip-pitched at θT = 2◦, the wake shape is axisymmetric, while a non-axisymmetric wake is observed for a single-rotor tip-pitched at θT = −2◦ and a dual-rotor with rotorspacing of 4D.330 Fig. 19 presents side view of the turbulence intensity of a single and dual-rotors operating at TSR 5 with ambient turbulence intensity of 1%. 

Mycek’s experimental work [27] showed that a maximum reduction of 13% in CP was observed when the ambient turbulence intensity increased from a low value of 3% to a high value of 15%. 

For a wind farm, the numerical results from Vaselbehagh [7] showed that the dual-rotor turbines produced 22.6% more power than the single-rotor turbines. 

For a dual-rotor with X=4D, an interesting observation is that a turbulence intensity region is developed in front of rear rotor. 

The value of the empirical wake expansion rate, k, is an important parameter for the velocity deficit calculation in the Park model.